Abstract
The qualitative features of the deformation energy of a charged drop are discussed with special reference to the fission process. It is shown that, under conditions more general than the model of an incompressible liquid drop with a sharp surface, the threshold energy for fission should be proportional to [(Z2A)0(Z2A)]3 near the limit of stability (Z2A)0. Similarly, if instability against asymmetry sets in below (Z2A)c, the degree of asymmetry of the asymmetric saddle-point shapes which appear should be proportional to [(Z2A)c(Z2A)]12 and the difference between the symmetric and asymmetric thresholds should be proportional to [(Z2A)c(Z2A)]2. Some factors governing the stability against asymmetry of a strongly deformed drop are discussed qualitatively.

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